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0 votes
0 answers
30 views

Is the tensor product involved in the metric a symmetric product?

The expression of the FRW metric in Cosmology in usually written as: $$ds^2=-dt^2+a^2(t)d\vec{x}^2$$ where $c=1$. However, $dt^2$ is a shortening of $dt\otimes dt$, that is, of the tensor product of $...
Wild Feather's user avatar
0 votes
1 answer
36 views

Question coming from Cosmological Perturbation

We consider the following scalar perturbation on the FRW metric: $$ ds^2 = -(1 + 2\phi)dt^2 +2a\partial_i B dx^i dt + a^2 \left( (1 - 2\psi)\delta_{ij} + 2\partial_{ij}E\right) dx^i dx^j $$ where $\...
Shivam Mishra's user avatar
0 votes
0 answers
86 views

Is there a metric, a solution to Einstein's field equations, for a single body in a space of uniform non-zero density?

The Swarzschild metric describes a single body in an empty space with zero density, while the FLRW metric is presumably for a space with uniform non-zero density but no single body. But is there a ...
John Hobson's user avatar
1 vote
2 answers
133 views

Is the FRW metric, based on spatial homogeneity and isotropy, rotationally and translationally invariant? If so, how?

The spatial part of the Minkowski metric, written in the Cartesian coordinates, $$d\vec{ x}^2=dx^2+dy^2+dz^2,$$ is invariant under spatial translations: $\vec{x}\to \vec{x}+\vec{a}$, where $\vec{a}$ ...
Solidification's user avatar
2 votes
1 answer
110 views

Saddle Shaped Universe

The universe, as described by FLRW metric, if $k = -1$ is clearly a 2 sheet 3-hyperboloid described by $x^2+y^2+z^2-w^2=-R^2$. So where does the more common saddle shaped picture of the open universe ...
Nayeem1's user avatar
  • 1,161
0 votes
2 answers
68 views

Homogeneous and Isotropic But not Maximally Symmetric Space

Is this statement correct: "In a homogeneous and Isotropic space the sectional curvature is constant, while in a maximally symmetric space the Riemann Curvature Tensor is covariantly constant in ...
Nayeem1's user avatar
  • 1,161
4 votes
3 answers
199 views

Change of variables from FRW metric to Newtonian gauge

My question arises from a physics paper, where they state that if we take the FRW metric as follows, where $t_c$ and $\vec{x}$ are the FRW comoving coordinates: $$ds^2=-dt_c^2+a^2(t_c)d\vec{x}_c^2$$ ...
Wild Feather's user avatar
0 votes
0 answers
27 views

A question about Friedmann cosmological expansion equation

A recent paper, arXiv:2403.01555, gives the equations for homogeneity and isotropy of an expanding 3-space as expressed in the following distance interval as $x^i = (t, \chi, \theta, \phi)$ and $x^i + ...
jim akerlund's user avatar
0 votes
1 answer
66 views

Name of metric used by Friedmann

In his original paper, Friedmann used the following dynamic and symmetrical metric: $$\mathrm{d}s^2=a(t)^2\left(\mathrm{d}\chi^2+\sin (\chi)^2\left(\mathrm{d}\theta^2+\sin (\theta)^2 \mathrm{d}\phi^2\...
Vincent ISOZ's user avatar
2 votes
0 answers
120 views

Transformation under coordinate transformation of scalar perurbation of FLRW metric

For the past few days I've been studying perturbation in cosmology. More specifically I am now busy with chapter 6 in Dodelson's Modern cosmology. In this book the perturbed FLRW metric which only ...
luki luk's user avatar
1 vote
0 answers
60 views

Robertson-Walker metric exercise [closed]

I'm trying to solve an exercise from my astrophysics and cosmology class, the request is the following, starting from the RW metric expression: $$ \begin{equation*} ds^2=c^2 dt^2 - a^2 \left ( \frac{...
Lip's user avatar
  • 41
1 vote
0 answers
88 views

Why is $h_{\mu\nu}$ not a tensor in the perturbed Universe in cosmological perturbation theory?

In the cosmological perturbation theory course per Hannu Kurki-Suonio (2022) : https://www.mv.helsinki.fi/home/hkurkisu/CosPer.pdf, there is a remark in the text page 5 that puzzles me. The text goes ...
Vincent's user avatar
  • 1,109
1 vote
1 answer
148 views

Deriving Klein-Gordon equation in curved spacetime [closed]

I try to drive The Klein-Gordon equation for a massless scalar field in case of FRW metric: $$ ds^2= a^2(t) [-dt^2 + dx^2] $$ So I start by: $$\left(\frac{1}{g^{1/2}}\partial_{\mu}(g^{1/2}g^{\mu\nu}\...
Dr. phy's user avatar
  • 395
4 votes
2 answers
170 views

Why isn't the curvature scale in Robertson-Walker metric dynamic?

$$ds^2=-c^2dt^2+a(t)^2 \left[ {dr^2\over1-k{r^2\over R_0^2}}+r^2d\Omega^2 \right]$$ This is the FRW metric, here k=0 for flat space, k=1 for spherical space, k=-1 for hyperbolic space. $R_0$ is the ...
Bababeluma's user avatar
0 votes
0 answers
230 views

Deriving the Ricci tensor on the flat FLRW metric

I am currently with a difficulty in deriving the space-space components of the Ricci tensor in the flat FLRW metric $$ds^2 = -c^2dt^2 + a^2(t)[dx^2 + dy^2 + dz^2],$$ to find: $$R_{ij} = \delta_{ij}[2\...
gabriel's user avatar

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